Abstract:We show how in the framework of the multimode Brownian oscillator model the system-bath correlation function can be derived from conventional and time-gated stimulated photon echo experiments and consideration of the linear optical spectra. Experiments are performed on the infrared dye DTTCI in room temperature solutions of ethylene glycol, methanol, and acetonitrile. The obtained correlation function is the sum of several Brownian oscillators, of which four are attributed to intrachromophore vibrational dynam… Show more
“…83,[85][86][87] Our previous experiments on dyes, however, showed this generally not to be the case. 8 Figure 4 shows that the spectral content of C(ω) agrees rather favorably with the unpolarized Raman spectrum of the highest frequency librational band of neat water 84,88,89 (note that the Raman spectrum of water in Figure 4 is multiplied by ω to allow a direct comparison with the spectral density 91 ). We note that a librational mode of similar frequency was found in model calculations on solvation dynamics in water by Hsu et al 12 We also note that the exponential part of our correlation function is identical to the one reported by Schwartz and Rossky.…”
Section: M′′(t)mentioning
confidence: 70%
“…In this model the Stokes shift (the gap between the first moments of emission and absorption) of the electronic transition is 2λ, provided that the excited-state lifetime is large compared to the solvation time. 8 This condition might not be fulfilled for the hydrated electron because of its extremely short excited-state lifetime. The calculations are rigorously carried out taking all possible time orderings and the finite pulse duration into account.…”
Section: Model Calculations For the Pump-probementioning
Hydrated-electron dynamics is examined by frequency-resolved pump-probe experiments using pulses of 13 fs centered at 780 nm. A recurrence at ∼40 fs signifies a strong coupling of the electronic transition to underdamped solvent motions. Wave packet dynamics launched by the pump pulse produces an ultrafast red-shift of the electronic transition by approximately 6500 cm -1 . Gross features of the pump-probe experiments are analyzed using a two-level system.
“…83,[85][86][87] Our previous experiments on dyes, however, showed this generally not to be the case. 8 Figure 4 shows that the spectral content of C(ω) agrees rather favorably with the unpolarized Raman spectrum of the highest frequency librational band of neat water 84,88,89 (note that the Raman spectrum of water in Figure 4 is multiplied by ω to allow a direct comparison with the spectral density 91 ). We note that a librational mode of similar frequency was found in model calculations on solvation dynamics in water by Hsu et al 12 We also note that the exponential part of our correlation function is identical to the one reported by Schwartz and Rossky.…”
Section: M′′(t)mentioning
confidence: 70%
“…In this model the Stokes shift (the gap between the first moments of emission and absorption) of the electronic transition is 2λ, provided that the excited-state lifetime is large compared to the solvation time. 8 This condition might not be fulfilled for the hydrated electron because of its extremely short excited-state lifetime. The calculations are rigorously carried out taking all possible time orderings and the finite pulse duration into account.…”
Section: Model Calculations For the Pump-probementioning
Hydrated-electron dynamics is examined by frequency-resolved pump-probe experiments using pulses of 13 fs centered at 780 nm. A recurrence at ∼40 fs signifies a strong coupling of the electronic transition to underdamped solvent motions. Wave packet dynamics launched by the pump pulse produces an ultrafast red-shift of the electronic transition by approximately 6500 cm -1 . Gross features of the pump-probe experiments are analyzed using a two-level system.
“…The Fleming and Wiersma groups have argued that one measurement, the photon echo peak shift (PEPS), strongly reflects the correlation function M(t). 4,5 A PEPS measurement involves taking a series of photon echo measurements for different fixed values of T 23 . Each photon echo measurement has a signal maximum at a particular value of T 12 .…”
Section: Physical Meaning Of the Photon Echo Peak Shiftmentioning
confidence: 99%
“…This has already been shown for certain carbocyanine dye molecules. 4,5 In this paper, we test this assumption for bacteriochloropyll a . …”
Section: Physical Meaning Of the Photon Echo Peak Shiftmentioning
confidence: 99%
“…Several groups have taken advantage of these ultrashort pulses to perform third-order optical coherence measurements of chromophores dissolved in solvents at room temperature. 3,4,5 In parallel to these experimental developments, Mukamel and co-workers have developed a theoretical picture, based on time correlation functions for the energy gap between optical states, that gives insight into the dynamical processes that underlie the experimental data. 6 This paper describes a method to extract correlation functions that reveal the dynamics of a chromophore in liquid solution from optical coherence measurements.…”
We present a method to determine system-bath correlation functions from third order optical coherence measurements. The importance of these correlation functions for understanding solvation dynamics is explained. A physical argument is made to explain why one coherence measurement, the photon echo peak shift, should strongly reflect system-bath dynamics. Finally, this method is applied to the system of bacteriochlorophyll a in tetrahydrofuran solution.
Fluorescence lineshape analysis based on resonance Raman spectra of the dye HITCI was used to determine the details and magnitude of the vibrational part of the line broadening function. Forced light scattering (FLS) was applied to measure optical dephasing of HITCI in ethylene glycol, pumping at 770 nm with 20 fs pulses from a Ti :sapphire laser and probing with continuous-wave light from an argon ion laser. The observed response is well described by the line broadening function derived from the Ñuorescence lineshape. High-frequency vibrational modes not covered directly by the laser spectrum account for 20% of the vibration-induced broadening in the FLS experiment. This e †ect is explained by di †erence frequency mixing with thermally populated low-frequency vibrations.
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